During polarized beam experiments, the 50 GeV proton synchrotron, proposed by the Institute of Nuclear Study of Japan, requires zero-dispersion straight sections. This will be implemented by turning on a special excitation of the quadrupoles resulting in a dispersion wave through the arcs of the machine. Aside from the inconvenience of the power supply, this special excitation also brings about unwanted high betatron functions and high dispersion functions, which will eventually limit the performance of the accelerator at high intensities. In this paper, dispersion suppressors are introduced. A new preliminary lattice that contains two straight sections with nonzero dispersion and two straight sections with zero dispersion is presented. The...
A proton synchrotron dedicated to medicaluse with the maximum energy of 250MeV has been designed. A ...
A description is given of an apparatus for the dynamic polarization of protons in a field of 50 kG. ...
In recent years, new precision experiments have become possible withthe high luminosity accelerator ...
Rapid cycling synchrotrons are used to accelerate high-intensity proton beams to energies of tens of...
Several kinds of lattice structures have been designed and examined for the JHF synchrotorons. The h...
A resent progress report on the lattice design of the 50-50 GeV muon collider is presented. The ring...
proposed to be built as a spallation neutron source at Centre for Advanced Technology. A lattice wit...
International audienceThe Gamma Factory proof of principle experiment aims at colliding laser pulses...
At present the new proton synchrotron PS2 with the energy range 4-50 GeV is discussed to upgrade LHC...
Rapid cycling synchrotrons are used to accelerate high-intensity proton beams to energies of tens of...
The goal of this manuscript is to give an introduction into the design of the magnet lattice and as ...
A possible method to realize a dispersion-free storage ring is described. The simultaneous use of a ...
A bipolar {gamma}{sub t}-jump design is reported for the Fermilab Main Injector (Lattice MI-17). The...
Abstract The Fermilab Main Injector (MI) accelerator is designed as a FODO lattice with zero dispers...
The Fermilab Main Injector (MI) accelerator is designed as a FODO lattice with zero dispersion strai...
A proton synchrotron dedicated to medicaluse with the maximum energy of 250MeV has been designed. A ...
A description is given of an apparatus for the dynamic polarization of protons in a field of 50 kG. ...
In recent years, new precision experiments have become possible withthe high luminosity accelerator ...
Rapid cycling synchrotrons are used to accelerate high-intensity proton beams to energies of tens of...
Several kinds of lattice structures have been designed and examined for the JHF synchrotorons. The h...
A resent progress report on the lattice design of the 50-50 GeV muon collider is presented. The ring...
proposed to be built as a spallation neutron source at Centre for Advanced Technology. A lattice wit...
International audienceThe Gamma Factory proof of principle experiment aims at colliding laser pulses...
At present the new proton synchrotron PS2 with the energy range 4-50 GeV is discussed to upgrade LHC...
Rapid cycling synchrotrons are used to accelerate high-intensity proton beams to energies of tens of...
The goal of this manuscript is to give an introduction into the design of the magnet lattice and as ...
A possible method to realize a dispersion-free storage ring is described. The simultaneous use of a ...
A bipolar {gamma}{sub t}-jump design is reported for the Fermilab Main Injector (Lattice MI-17). The...
Abstract The Fermilab Main Injector (MI) accelerator is designed as a FODO lattice with zero dispers...
The Fermilab Main Injector (MI) accelerator is designed as a FODO lattice with zero dispersion strai...
A proton synchrotron dedicated to medicaluse with the maximum energy of 250MeV has been designed. A ...
A description is given of an apparatus for the dynamic polarization of protons in a field of 50 kG. ...
In recent years, new precision experiments have become possible withthe high luminosity accelerator ...